1 / 16

Exploring Neutrinos from Kaon Decay in MiniBooNE Experiment

MiniBooNE at Columbia University searches for nm to ne oscillations by producing a beam of neutrinos from kaon decays. The experiment involves measuring kaons through muons and neutrino events, analyzing high-energy neutrino interactions, and selecting neutrino events in the MiniBooNE detector.

louisel
Download Presentation

Exploring Neutrinos from Kaon Decay in MiniBooNE Experiment

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Neutrinos from kaon decay in MiniBooNEKendall MahnColumbia University • MiniBooNE beamline overview • Kaon flux predictions • Kaon measurements in MiniBooNE • high energy events • Summary

  2. MiniBooNE beamline • MiniBooNE is searching for nm to ne oscillations • Produce a beam of nm, look for ne • 8 GeV protons hit Be target, producing: • p+ (primary source of nm ) • K+/- (decay to nm, ne) • K0 (decay to ne )

  3. Oscillation search backgrounds ne p0 • Three major backgrounds: • misID’d p0s • constrained by observed p0s • nefrom muon decay • muon produced for each nm, constrained via nm spectrum • nefrom kaon decay nm m+ e+ p+ ne nm ne K+, K0

  4. K+ flux predictions • All flux predictions are from a parameterized fit to external data with uncorrelated uncertainties • K+ external data shown here in transverse momentum (pT ) vs x F • Feynman x, the longitudinal momentum / maximum allowed longitudinal momentum • Currently use Aleshin, Abbot, Eichten, Piroue and Vorontsov data p T (GeV/C) x F

  5. Measurements of kaons in MiniBooNE • MiniBooNE is a blinded analysis: • we can’t look at ne -like events at energies where there might be oscillation events • must measure kaons outside the signal region and extrapolate

  6. Measurements of kaons in MiniBooNE • Measure kaons via muons: Little Muon Counter (LMC) • Large angle muons are predominantly from kaon decays (higher allowed pT for muons from kaons) • Count muons at 7o angle from decay pipe and determine corresponding kaon rate • Measure kaons via neutrino events: high energy “box” • A neutrino from a kaon will have a higher energy than if it came from a pion of the same momentum • Highest energy tank events tend to be from K+ • Directly measure ne background in different energy region

  7. Neutrino Events in MiniBooNE • 12 m diameter light detector filled with mineral oil • 1280 PMTs in inner region • 240 PMTs in outer “veto” region • Neutrino events emit Cherenkov light in a characteristic pattern for different events • Muons have long tracks, constant light over distance • Electrons have shorter tracks; scattering causes the ring to be “fuzzier” e m

  8. Neutrino Interactions • Charged Current Quasi-elastic (CCQE) • Energy of neutrino is related to the outgoing leptons’ energy and angle l+ nl • mpEl - ml2/2 • En(QE)= p • mp - El + √(El2 -ml2) cos qm n • Charged Current Pion production (CCp) l nl C p+ X

  9. High Energy Box Event selection: • Event is in time with the beam • Has a En(QE) (assuming muon) > 1.5 GeV, < 4 GeV • Passes cosmic ray reduction cuts • within forward cone along the beam direction • Veto hits less than 30 • Entering cluster hits less than 1 • Less than 1 hit in the veto corresponding to the track direction m x x x m nm

  10. High Energy Box Monte Carlo p+ K+ K0, m,p- Predominantly p+ below 2 GeV, predominantly K+ above En (QE) in GeV 1.5 GeV

  11. High Energy Box: nm events Preliminary • Look at CCQE, CC p+nm events as a check of p+, K+ • long tracks consistent with muon • veto hits<6 (contained) Total MC Data(stat only) p +K+ Note: All plots are relatively normalized to 1 Absolutely normalized plots show a normalization difference of ~50% => MiniBooNE is working on this 1.5 GeV En(QE) in GeV logarithmic scale

  12. High Energy Box: nm events Preliminary • Look at CCQE, CC p+nm events as a check of p+, K+ • long tracks consistent with muon • veto hits<6 (contained) Total MC Data(stat only) CCQE CC p + Note: All plots are relatively normalized to 1 Absolutely normalized plots show a normalization difference of ~50% => MiniBooNE is working on this 1.5 GeV En(QE) in GeV logarithmic scale

  13. High Energy Box: ne events • Look at CCQE ne events as a check of all ne backgrounds • run the ne PID prepared for the oscillation analysis on this sample Preliminary Preliminary Oscillation K+ misIDK0 m p+HE box data (stat only) En(QE) (electron) GeV

  14. High Energy Box: ne events • Look at CCQE ne events as a check of all ne backgrounds • run the ne PID prepared for the oscillation analysis on this sample Preliminary Oscillation K+ misIDK0 m p+ HE box data (stat only, 3.25e20 pot) En(QE) (electron) GeV

  15. Using the HE box • The different event samples in the HE provide checks of the predicted neutrino from kaon rate • Example: CCQE contained events: • 2 subevents, decay michel electron energy <70 MeV, veto hits < 6, muon-like track • ~11K data events for 5e20 pot, 82% CCQE, 15% CCp • 17% error due to cross sections, 5% due to flux, 7% optical model

  16. Summary • MiniBooNE is searching for nm to ne oscillations • Observing these oscillations depends on understanding the content of the neutrino beam • The HE box and LMC provide MiniBooNE with checks using the same beamline of the kaons • Check of K+ m from the LMC • Check of p+, K+ nm from HE box CCQE, CCpi muon-like events • Check of K0, K+ ne from HE box CCQE electron-like events

More Related